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4.1. Resultados

4.1.3. Procedimientos para elaboración de la propuesta económica

The ultimate loads calculation, which is often required for certification calculations, is simple in concept: the results of a load case simulation are analysed to find the times at which each of a number of specified loads reaches its maximum and minimum values. The simultaneous values of all the loads at each of those instants is reported.

A further calculation named ‘ultimate load cases’ further analyses the results of a number of ultimate loads calculations for different groups of load cases, and generates a histogram showing the load cases in which the maximum and minimum values of each load occurred within each group.

9.9 Flicker

The Flicker calculation generates short-term flicker severity values (Pst), either from a voltage time history, or from time histories of active and reactive power. Such time histories are available from simulations with the full electrical model of the fixed speed induction generator, and also with the variable speed generator model.

The flicker severity is a measure of the annoyance created by voltage variations through perception of the resulting flicker of incandescent lights. The calculation of flicker from a voltage time history is defined in [9.5]. An algorithm conforming to this standard is incorporated into the Bladed post-processor. It can also calculate flicker from a time history of active and reactive power. In this case a voltage time history is calculated first, and this can be calculated for any given network impedance to which the wind turbine might be connected. In fact the flicker for several different network impedances can be calculated in a single calculation. The network impedances are entered as a set of short circuit power levels and network angles, the network angle being arctan(X/R), where X and R are the network reactance and resistance respectively. The voltage is calculated as the solution of the following equation:

U4+ U2(2{QX - PR} - U

02) + (QX - PR)2+ (PX + QR)2= 0

where U0 is the voltage at the infinite busbar, and P and Q are the active and reactive power respectively.

10. REFERENCES

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ETSU WN 6018, ETSU, 1991.

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7.5 Engineering Sciences Data Unit, “Characteristics of atmospheric turbulence near the ground. Part II: Single point data for strong winds (neutral atmosphere)”, ESDU 85020, 1985 (amended 1993).

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7.7 IEC 1400-1, Wind turbine generator systems - Part 1: Safety requirements, Second edition, 1997.

7.8 Ainslie J F, “Development of an eddy viscosity model for wind turbine wakes”, Proceedings of 7th BWEA Wind Energy Conference, Oxford 1985.

7.9 Ainslie J F, “Development of an Eddy Viscosity model of a Wind Turbine Wake”, CERL Memorandum TPRD/L/AP/0081/M83, 1983.

7.10 H Tennekes and J Lumley, “A first course in turbulence”, MIT Press, 1980. 7.11 L Prandtl, “Bemerkungen zur Theorie der freien Turbulenz”, ZAMM, 22(5), 1942. 7.12 Ainslie J F, “Calculating the flowfield in the wake of wind turbines”, Journal of Wind

Engineering and Industrial Aerodynamics, Vol 27, 1988.

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7.15 U Hassan, “A Wind Tunnel Investigation of the Wake Structure within Small Wind Turbine Farms”, Department of Energy, E/5A/CON/5113/1890, 1992.

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7.17 Vermeulen P and Vijge J, “Mathematical Modelling of Wake Interaction in Wind Turbine Arrays, Part2”, report TNO 81-02834, 1981.

8.1 Goda Y, “A Review on Statistical Interpolation of Wave Data”, Report of the Port and Harbour Research Institute, Vol. 18, No. 1, March 1979.

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8.4 Gudmestad O T, “Measured and Predicted Deep Water Wave Kinematics in Regular and Irregular Seas”, Marine Structures, Vol. 6, pp.1-73, 1993.

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9.5 Flickermeter functional and design specification, BSEN60868, 1993, and evaluation of flicker severity, BSEN60868-0, 1993, equivalent to IEC 868-0, 1991.

In document UNIVERSIDAD PERUANA LOS ANDES (página 67-0)